NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = C.Bourrely Found 14 matches. 2019BO01 Nucl.Phys. A981, 118 (2019) Statistical approach of pion parton distributions from Drell-Yan process
doi: 10.1016/j.nuclphysa.2018.07.003
2019SO19 Nucl.Phys. A991, 121607 (2019) On the flavor structure of the light-quark sea distributions
doi: 10.1016/j.nuclphysa.2019.08.001
2018BO23 Phys.Rev. C 98, 055202 (2018) Properties of structure functions from helicity components of light quarks and antiquarks in the statistical model
doi: 10.1103/PhysRevC.98.055202
2017BA20 Nucl.Phys. A966, 113 (2017) E.Basso, C.Bourrely, R.Pasechnik, J.Soffer The landscape of W± and Z bosons produced in pp collisions up to LHC energies
doi: 10.1016/j.nuclphysa.2017.06.035
2016BA11 Nucl.Phys. A948, 63 (2016) E.Basso, C.Bourrely, R.Pasechnik, J.Soffer The Drell-Yan process as a testing ground for parton distributions up to LHC
doi: 10.1016/j.nuclphysa.2016.02.001
2015BO09 Nucl.Phys. A941, 307 (2015) New developments in the statistical approach of parton distributions: Tests and predictions up to LHC energies
doi: 10.1016/j.nuclphysa.2015.06.018
2007BO11 Phys.Lett. B 648, 39 (2007) C.Bourrely, J.Soffer, F.Buccella Strangeness asymmetry of the nucleon in the statistical parton model NUCLEAR REACTIONS Fe(ν, X), E=90.2, 109.46, 174.4, 209.89, 244.7, 332.7 GeV; Fe(ν-bar, X), E=78.98, 87.4, 146.06, 160.52, 222.14, 265.76 GeV; analysed strange quark-antiquark distributions. Statistical parton model.
doi: 10.1016/j.physletb.2007.02.063
2004BO25 Eur.Phys.J. C 36, 371 (2004) Do we understand the single-spin asymmetry for π0 inclusive production in pp collisions? NUCLEAR REACTIONS 1H(polarized p, π0X), E=high; analyzed σ(E, θ), single-spin asymmetry.
doi: 10.1140/epjc/s2004-01956-4
2003BO12 Eur.Phys.J. C 28, 97 (2003) Impact-picture phenomenology for π±p, K±p and pp, (p-bar)p elastic scattering at high energies NUCLEAR REACTIONS 1H(p, p), (p-bar, p-bar), (π+, π+), (π-, π-), (K+, K+), (K-, K-), E=high; calculated σ(E, θ). Impact-picture phenomenology.
doi: 10.1140/epjc/s2003-01159-7
2002BO14 Eur.Phys.J. C 23, 487 (2002) C.Bourrely, J.Soffer, F.Buccella A Statistical Approach for Polarized Parton Distributions NUCLEAR STRUCTURE 1H; analyzed structure functions, polarized parton distributions. Statistical approach. NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=350, 500 GeV; calculated W, Z production associated asymmetries.
doi: 10.1007/s100520100855
1998BO25 Prog.Theor.Phys.(Kyoto) 99, 1017 (1998) C.Bourrely, F.Buccella, O.Pisanti, P.Santorelli, J.Soffer Polarized Quarks, Gluons and Sea in Nucleon Structure Functions NUCLEAR REACTIONS 1H(e, e'X), E not given; analyzed data; deduced structure function parameters, relative merits of spin crisis solutions.
doi: 10.1143/PTP.99.1017
1998BO34 Phys.Lett. 442B, 479 (1998) Proton-Helium Elastic Scattering: A possible high-energy polarimeter at RHIC-BNL NUCLEAR REACTIONS 4He(polarized p, p), E=393 GeV; analyzed σ(t), single-spin asymmetry; deduced theoretical uncertainties, unsuitability as absolute polarimeter. Coulomb-nuclear interference effect.
doi: 10.1016/S0370-2693(98)01272-6
1994BO42 Phys.Lett. 339B, 322 (1994) Expanding Protons Seen by HERA NUCLEAR REACTIONS 1H(γ, X), E=high; calculated σ vs E(cm); deduced expanding protons related features.
doi: 10.1016/0370-2693(94)90627-0
1994BO55 Nucl.Phys. B423, 329 (1994) Parton Distributions from W± and Z Production in Polarized pp and pn Collisions at RHIC NUCLEAR REACTIONS 1n, 1H(polarized p, X), E=relativistic; calculated parton distribution from W+, W-, Z production, relativistic energies.
doi: 10.1016/0550-3213(94)90137-6
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